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    贾剑平, 李田雨. 冷金属过渡电弧增材制造5183铝合金温度场的数值模拟[J]. 机械工程材料, 2024, 48(1): 106-111. DOI: 10.11973/jxgccl202401017
    引用本文: 贾剑平, 李田雨. 冷金属过渡电弧增材制造5183铝合金温度场的数值模拟[J]. 机械工程材料, 2024, 48(1): 106-111. DOI: 10.11973/jxgccl202401017
    JIA Jianping, LI Tianyu. Numerical Simulation of Temperature Field of Cold Metal Transition Arc Additive Manufacturing 5183 Aluminum Alloy[J]. Materials and Mechanical Engineering, 2024, 48(1): 106-111. DOI: 10.11973/jxgccl202401017
    Citation: JIA Jianping, LI Tianyu. Numerical Simulation of Temperature Field of Cold Metal Transition Arc Additive Manufacturing 5183 Aluminum Alloy[J]. Materials and Mechanical Engineering, 2024, 48(1): 106-111. DOI: 10.11973/jxgccl202401017

    冷金属过渡电弧增材制造5183铝合金温度场的数值模拟

    Numerical Simulation of Temperature Field of Cold Metal Transition Arc Additive Manufacturing 5183 Aluminum Alloy

    • 摘要: 利用有限元分析软件ABAQUS使用生死单元法建立冷金属过渡(CMT)电弧增材制造单道10层5183铝合金模型,模拟分析了增材制造过程中温度场的分布和变化规律,并进行试验验证;采用该模拟方法研究了增材制造路径(单向和交叉路径)、层间冷却时间(20,40,60 s)和焊接速度(400,450,500 mm·min-1)对温度场的影响。结果表明:模拟得到在CMT电弧增材制造过程中基板某点的热循环曲线的变化趋势与试验结果基本一致,且峰值温度和波谷温度与试验结果的相对误差均不大于8.93%,验证了模型的准确性。随着堆焊层数的增加,熔池峰值温度升高,熔池区域变大;单向路径增材制造会在试样收弧端产生较严重的热积累,而交叉路径可以减弱热积累效应;层间冷却时间越长,焊道中点的峰值温度越低,且降低幅度随冷却时间的延长而逐渐减弱;焊道的峰值温度和波谷温度随焊接速度的增加而降低。

       

      Abstract: The finite element analysis software ABAQUS was used to establish the model of cold metal transition (CMT) arc additive manufacturing single-pass ten-layer 5183 aluminum alloy by the birth and death element method. The distribution and variation of temperature during the additive process were simulated and analyzed, and was verified by experiments. The effects of additive manufacture path (unidirectional path and cross path), interlayer cooling time interval (20,40,60 s) and welding speed (400, 450, 500 mm·min-1) on the temperature field were studied by simulation. The results show that the variation trend of the thermal cycle curve at one point on the substrate obtained by simulation was basically consistent with the test results in the CMT arc additive manufacturing process, and the relative errors between peak temperature or bottom temperature and test results were both not larger than 8.93%, verifying the accuracy of the model. With the increase of the number of surfacing layers, the peak temperature and the area of the molten pool increased. The unidirectional path additive manufacturing could produce serious heat accumulation at the ending arc of the sample, while the cross path could weaken the heat accumulation effect. The longer the interlayer cooling time interval, the lower the peak temperature at the midpoint of the weld bead; the reduction amplitude gradually decreased with the extension of the cooling time interval. The peak temperature and bottom temperature of weld bead decreased with the increase of welding speed.

       

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